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首页> 外文期刊>Journal of radiation research >A comparison of the dose distributions between the brachytherapy 125I source models, STM1251 and Oncoseed 6711, in a geometry lacking radiation equilibrium scatter conditions
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A comparison of the dose distributions between the brachytherapy 125I source models, STM1251 and Oncoseed 6711, in a geometry lacking radiation equilibrium scatter conditions

机译:在缺乏辐射平衡散射条件的几何结构中,近距离放射治疗125I放射源模型STM1251和Oncoseed 6711之间的剂量分布比较

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As the procedure has previously been detailed in [10], it is described briefly here. Dosimeters were irradiated with an 125I source ‘BARD STM1251' (Bard Inc., Murray Hill, NJ). The source was calibrated by the manufacturer with a stated air kerma strength of 0.317 U at the beginning of irradiation. The dosimeters used in this work were radiophotoluminescent glass rod dosimeters (GRDs) model GD-302M (Asahi Techno Glass Corporation, Shizuoka). The GRDs were calibrated in advance using a 6-MV X-ray beam from a linear accelerator (Primus KD2/7467, Toshiba Corporation, Tokyo). Calculations were carried out using the Monte Carlo (MC) code EGS5 [12]. The absorbed dose to the GRDs was calculated for the same geometry as the GRD measurement. The EGS5 output was then converted to an absorbed dose to water using the mass energy-absorption coefficient [11]. The calculation geometry included the 125I source, GRDs and the phantom placed on a Styrofoam block (25 × 25 × 20 cm thickness) and Pb (90 × 90 × 6 cm thickness). The geometry input for the 125I source (STM1251) was the same as that used by Kirov et al. [13]. The dose uncertainty for STM1251 was estimated in a manner similar to that of the Oncoseed 6711 investigation [7]. The dose uncertainties for each of the uncertainty components were combined in quadrature to obtain the Combined Standard Uncertainty (CSU) for the coverage factor k, set at 1.
机译:由于该过程先前已在[10]中进行了详细介绍,因此在此进行简要说明。用 125 I光源“ BARD STM1251”(Bard Inc.,Murray Hill,NJ)辐照剂量计。光源由制造商校准,辐照开始时标称空气比释动能强度为0.317U。这项工作中使用的剂量计是型号GD-302M的放射光致发光玻璃棒剂量计(GRD)(静冈旭化成玻璃公司)。预先使用来自线性加速器(Primus KD2 / 7467,东芝公司,东京)的6-MV X射线束对GRD进行校准。使用蒙特卡罗(MC)代码EGS5 [12]进行计算。对于与GRD测量相同的几何形状,计算到GRD的吸收剂量。然后使用质量能量吸收系数[11]将EGS5的输出转换为对水的吸收剂量。计算几何形状包括 125 I源,GRD和放置在泡沫聚苯乙烯块(25×25×20 cm厚度)和Pb(90×90×6 cm厚度)上的体模。 125 I源(STM1251)的几何输入与Kirov等人使用的相同。 [13]。以类似于Oncoseed 6711研究[7]的方式估计STM1251的剂量不确定性。将每个不确定度分量的剂量不确定度进行正交组合,以获得覆盖因子k的组合标准不确定度(CSU),设置为1。

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